{"title":"高非线性、高双折射的超扁平负色散椭圆螺旋光子晶体光纤的设计","authors":"A. Ghunawat, Ritesh Chandra, G. Singh","doi":"10.1109/COMPTELIX.2017.8004044","DOIUrl":null,"url":null,"abstract":"Novel elliptical spiral photonic crystal fiber(PCF) having ultra-flattened negative dispersion, high nonlinearity and high birefringence is proposed. The finite element method is used to optimize the guiding properties. This design provides negative dispersion that is ultra-flattened within range of wavelength from 1385 nm to 1990 nm with deviation of ± 1.5 ps/nm/km. Dispersion value of −93.577 ps/nm/km at 1550 nm wavelength is achieved. The numerical results also indicate the birefringence up to order of 10−2 and nonlinear coefficient of (678.264, 763.485) W−1km−1 at 1550 nm wavelength for fundamental X and Y polarized modes.","PeriodicalId":6917,"journal":{"name":"2017 International Conference on Computer, Communications and Electronics (Comptelix)","volume":"70 1","pages":"623-627"},"PeriodicalIF":0.0000,"publicationDate":"2017-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"6","resultStr":"{\"title\":\"Design of an ultra-flattened negative dispersion elliptical spiral photonic crystal fiber with high nonlinearity and high birefringence\",\"authors\":\"A. Ghunawat, Ritesh Chandra, G. Singh\",\"doi\":\"10.1109/COMPTELIX.2017.8004044\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Novel elliptical spiral photonic crystal fiber(PCF) having ultra-flattened negative dispersion, high nonlinearity and high birefringence is proposed. The finite element method is used to optimize the guiding properties. This design provides negative dispersion that is ultra-flattened within range of wavelength from 1385 nm to 1990 nm with deviation of ± 1.5 ps/nm/km. Dispersion value of −93.577 ps/nm/km at 1550 nm wavelength is achieved. The numerical results also indicate the birefringence up to order of 10−2 and nonlinear coefficient of (678.264, 763.485) W−1km−1 at 1550 nm wavelength for fundamental X and Y polarized modes.\",\"PeriodicalId\":6917,\"journal\":{\"name\":\"2017 International Conference on Computer, Communications and Electronics (Comptelix)\",\"volume\":\"70 1\",\"pages\":\"623-627\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2017-07-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"6\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2017 International Conference on Computer, Communications and Electronics (Comptelix)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/COMPTELIX.2017.8004044\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2017 International Conference on Computer, Communications and Electronics (Comptelix)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/COMPTELIX.2017.8004044","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Design of an ultra-flattened negative dispersion elliptical spiral photonic crystal fiber with high nonlinearity and high birefringence
Novel elliptical spiral photonic crystal fiber(PCF) having ultra-flattened negative dispersion, high nonlinearity and high birefringence is proposed. The finite element method is used to optimize the guiding properties. This design provides negative dispersion that is ultra-flattened within range of wavelength from 1385 nm to 1990 nm with deviation of ± 1.5 ps/nm/km. Dispersion value of −93.577 ps/nm/km at 1550 nm wavelength is achieved. The numerical results also indicate the birefringence up to order of 10−2 and nonlinear coefficient of (678.264, 763.485) W−1km−1 at 1550 nm wavelength for fundamental X and Y polarized modes.